Semi-grand ensembles: Difference between revisions

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== Semi-grand ensemble at fixed volume and temperature ==
== Semi-grand ensemble at fixed volume and temperature ==
Consider now that we want to consider a system with fixed total number of particles, <math> N </math>
: <math> \left. N = N_1 + N_2 \right. </math>;
but the composition can change, from the thermodynamics we can apply a Legendre's transform [HAVE TO CHECK ACCURACY]
to the differential equation written above in terms of <math> A (T,V,N_1,N_2) </math>.
# Consider the change <math> (N_1,N_2) \rightarrow (N,N_2) </math>

Revision as of 14:08, 5 March 2007

General Features

Semi-grand ensembles are used in Monte Carlo simulation of mixtures.

In this ensembles the total number of molecules is fixed, but the composition can change.

Canonical Ensemble: fixed volume, temperature and number(s) of molecules

We will consider a binary system;. In the Canonical Ensemble, the differential equation energy for the Helmholtz energy function can be written as:

d(βA)=Edβ−(βp)dV+∑i=12(βμi)dNi,

where:

  • A is the Helmholtz energy function
  • β≡1/kBT
  • kB is the Boltzmann constant
  • T is the absolute temperature
  • E is the internal energy
  • p is the pressure
  • μi is the chemical potential of the species "i"
  • Ni is the number of molecules of the species "i"

Semi-grand ensemble at fixed volume and temperature

Consider now that we want to consider a system with fixed total number of particles, N

N=N1+N2;

but the composition can change, from the thermodynamics we can apply a Legendre's transform [HAVE TO CHECK ACCURACY] to the differential equation written above in terms of A(T,V,N1,N2).

  1. Consider the change (N1,N2)→(N,N2)